2020
DOI: 10.1140/epjp/s13360-019-00088-x
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The exponent of the longitudinal structure function $$F_{\text {L}}$$ at low x

Abstract: We present a set of formula to extract exponents of the longitudinal structure function and reduced cross section from the Regge-like behavior at small x. The exponents are found to be independent of Q 2 at NNLO analysis. As a result, we show that the reduced cross section exponents do not have the same behavior at some values of x. This difference predicts the non-linear effects and some evidence for shadowing and antishadowing at LHeC. Also the ratio F 2 σ is calculated and compared with the corresponding HE… Show more

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Cited by 7 publications
(1 citation statement)
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“…The gluon exponent at low values of is described by the hard pomeron, as the fixed coupling LLx BFKL solution gives the value , although dependence on is expressed in the effective exponent defined in Refs. [55][56][57][58]. In the literature, fits to experimental data suggest that hard pomerons dominate the behavior of the heavy quark structure function.…”
Section: G→qq Xmentioning
confidence: 99%
“…The gluon exponent at low values of is described by the hard pomeron, as the fixed coupling LLx BFKL solution gives the value , although dependence on is expressed in the effective exponent defined in Refs. [55][56][57][58]. In the literature, fits to experimental data suggest that hard pomerons dominate the behavior of the heavy quark structure function.…”
Section: G→qq Xmentioning
confidence: 99%